supplementary materials


Acta Cryst. (2009). E65, o2147    [ doi:10.1107/S1600536809031419 ]

5-(2-Furyl)-3-methyl-1-(3-nitrophenyl)-4,5-dihydro-1H-pyrazole

J. Chen, H. Li, C. Huang and J. Wu

Abstract top

In the title compound, C14H13N3O3, the pyrazoline ring assumes an envelope conformation with the furanyl-bearing C atom at the flap position. The dihedral angle between the furan and nitrobenzene rings is 84.40 (9)°. Weak intermolecular C-H...O hydrogen bonding is present in the crystal structure.

Comment top

The derivatives of pyrazoline are mostly used in medicine, for example as antitumor (Hatheway et al., 1978), analgesic (Sobczak & Pawlaczyk, 1998), and antimicrobial (Mahajan et al., 1991) agents. As part of our work, the new title compound (I) are synthesized in our group.

The pyrazoline ring assumes an envelope conformation with the furanyl-bearing carbon atom at the flap position (Fig. 1). Intermolecular weak C—H···O hydrogen bonding is present in the crystal structure. (Fig. 2 and Table 1).

Related literature top

For applications of pyrazoline derivatives, see: Hatheway et al. (1978); Mahajan et al. (1991); Sobczak & Pawlaczyk (1998).

Experimental top

3-Nitrophenylhydrazine (1 mmol, 0.153 g) was dissolved in anhydrous ethanol (15 ml). The mixture was stirred for several min at 351 K, furylideneacetone (1 mmol, 0.136 g) in ethanol (8 mm l) was added dropwise and the mixture was stirred at refluxing temperature for 2 h. The product was isolated and recrystallized from methanol, bronze single crystals of (I) were obtained after 3 d.

Refinement top

All H atoms were positioned geometrically and refined as riding with C—H = 0.93 (aromatic), 0.97 (methylene), 0.98 (methine) and 0.96 Å (methyl), with Uiso(H)=1.5Ueq(C) for methyl H atoms and 1.2Ueq(C) for the others.

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. Packing of (I), showing the intermolecular hydrogen bonds as dashed lines.
5-(2-Furyl)-3-methyl-1-(3-nitrophenyl)-4,5-dihydro-1H-pyrazole top
Crystal data top
C14H13N3O3Z = 2
Mr = 271.27F(000) = 284
Triclinic, P1Dx = 1.362 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.2089 (2) ÅCell parameters from 1598 reflections
b = 7.8581 (3) Åθ = 3.5–24.6°
c = 14.3800 (4) ŵ = 0.10 mm1
α = 105.764 (2)°T = 296 K
β = 97.054 (2)°Block, bronze
γ = 96.944 (2)°0.31 × 0.15 × 0.10 mm
V = 661.31 (4) Å3
Data collection top
Bruker SMART CCD area-detector
diffractometer
1778 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.036
graphiteθmax = 26.0°, θmin = 3.5°
ω scansh = 77
9707 measured reflectionsk = 89
2590 independent reflectionsl = 1717
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.121H-atom parameters constrained
S = 1.10 w = 1/[σ2(Fo2) + (0.0608P)2]
where P = (Fo2 + 2Fc2)/3
2590 reflections(Δ/σ)max = 0.003
181 parametersΔρmax = 0.14 e Å3
0 restraintsΔρmin = 0.20 e Å3
Crystal data top
C14H13N3O3γ = 96.944 (2)°
Mr = 271.27V = 661.31 (4) Å3
Triclinic, P1Z = 2
a = 6.2089 (2) ÅMo Kα radiation
b = 7.8581 (3) ŵ = 0.10 mm1
c = 14.3800 (4) ÅT = 296 K
α = 105.764 (2)°0.31 × 0.15 × 0.10 mm
β = 97.054 (2)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
1778 reflections with I > 2σ(I)
9707 measured reflectionsRint = 0.036
2590 independent reflectionsθmax = 26.0°
Refinement top
R[F2 > 2σ(F2)] = 0.044H-atom parameters constrained
wR(F2) = 0.121Δρmax = 0.14 e Å3
S = 1.10Δρmin = 0.20 e Å3
2590 reflectionsAbsolute structure: ?
181 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O0.36743 (18)0.34679 (15)0.90208 (8)0.0586 (3)
N10.1661 (2)0.62239 (17)0.78604 (10)0.0496 (4)
N20.2000 (2)0.45740 (16)0.72794 (10)0.0491 (4)
C90.3755 (2)0.4521 (2)0.67745 (11)0.0429 (4)
C140.5059 (2)0.6102 (2)0.67820 (11)0.0460 (4)
H14A0.47720.72110.71320.055*
C70.0168 (3)0.5942 (2)0.83623 (13)0.0534 (4)
C100.4224 (3)0.2892 (2)0.62195 (12)0.0546 (4)
H10A0.33470.18260.61910.066*
C40.2531 (2)0.2318 (2)0.81601 (12)0.0477 (4)
C130.6784 (2)0.5987 (2)0.62600 (12)0.0514 (4)
N30.8105 (2)0.7665 (2)0.62761 (12)0.0680 (5)
O10.9707 (2)0.7615 (2)0.58611 (11)0.0934 (5)
C50.0941 (2)0.3072 (2)0.75855 (12)0.0508 (4)
H5A0.01380.21260.70100.061*
C120.7298 (3)0.4395 (3)0.57272 (12)0.0611 (5)
H12A0.84870.43650.53910.073*
C60.0684 (3)0.4007 (3)0.81836 (14)0.0615 (5)
H6A0.21660.36860.78170.074*
H6B0.06770.37060.87950.074*
C10.4967 (3)0.2476 (3)0.94299 (14)0.0607 (5)
H1B0.59240.29201.00220.073*
O20.7571 (3)0.9062 (2)0.67000 (14)0.1046 (6)
C110.5976 (3)0.2848 (3)0.57136 (13)0.0642 (5)
H11A0.62700.17480.53550.077*
C30.3090 (3)0.0707 (2)0.80439 (14)0.0660 (5)
H3A0.25500.03080.75180.079*
C20.4665 (3)0.0818 (3)0.88708 (14)0.0673 (5)
H2A0.53500.01080.89920.081*
C80.0654 (3)0.7433 (3)0.90245 (15)0.0793 (6)
H8A0.01410.85560.90190.119*
H8B0.04440.73290.96780.119*
H8C0.21910.73810.88060.119*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O0.0577 (7)0.0535 (7)0.0622 (8)0.0133 (5)0.0000 (6)0.0156 (6)
N10.0513 (8)0.0481 (8)0.0555 (8)0.0152 (6)0.0159 (6)0.0190 (7)
N20.0507 (7)0.0414 (7)0.0613 (9)0.0090 (6)0.0178 (6)0.0206 (7)
C90.0443 (8)0.0457 (9)0.0417 (9)0.0103 (7)0.0050 (7)0.0172 (7)
C140.0459 (8)0.0467 (9)0.0464 (9)0.0077 (7)0.0087 (7)0.0147 (7)
C70.0454 (8)0.0673 (11)0.0568 (10)0.0186 (8)0.0109 (8)0.0284 (9)
C100.0639 (10)0.0459 (10)0.0528 (10)0.0079 (8)0.0105 (8)0.0125 (8)
C40.0474 (8)0.0414 (9)0.0544 (10)0.0009 (7)0.0061 (7)0.0179 (8)
C130.0452 (9)0.0591 (10)0.0501 (10)0.0017 (8)0.0074 (7)0.0191 (8)
N30.0584 (9)0.0749 (12)0.0685 (10)0.0040 (8)0.0163 (8)0.0210 (9)
O10.0729 (9)0.1114 (12)0.0966 (11)0.0083 (8)0.0418 (8)0.0290 (9)
C50.0440 (8)0.0488 (9)0.0621 (10)0.0003 (7)0.0046 (7)0.0256 (8)
C120.0591 (10)0.0759 (13)0.0516 (11)0.0182 (9)0.0200 (8)0.0159 (9)
C60.0403 (8)0.0813 (13)0.0765 (12)0.0102 (8)0.0121 (8)0.0440 (11)
C10.0531 (10)0.0751 (13)0.0613 (11)0.0207 (9)0.0076 (8)0.0285 (10)
O20.0990 (12)0.0602 (9)0.1522 (16)0.0069 (8)0.0581 (11)0.0187 (10)
C110.0777 (12)0.0602 (11)0.0550 (11)0.0230 (10)0.0176 (10)0.0093 (9)
C30.0813 (13)0.0457 (10)0.0690 (13)0.0129 (9)0.0027 (10)0.0164 (9)
C20.0761 (12)0.0621 (13)0.0761 (13)0.0288 (10)0.0118 (10)0.0333 (11)
C80.0778 (13)0.0996 (16)0.0771 (14)0.0422 (12)0.0352 (11)0.0316 (12)
Geometric parameters (Å, °) top
O—C41.3689 (18)N3—O21.208 (2)
O—C11.372 (2)N3—O11.2209 (19)
N1—C71.277 (2)C5—C61.532 (2)
N1—N21.3940 (18)C5—H5A0.9800
N2—C91.3803 (19)C12—C111.376 (3)
N2—C51.4784 (19)C12—H12A0.9300
C9—C141.396 (2)C6—H6A0.9700
C9—C101.397 (2)C6—H6B0.9700
C14—C131.379 (2)C1—C21.309 (2)
C14—H14A0.9300C1—H1B0.9300
C7—C81.482 (2)C11—H11A0.9300
C7—C61.489 (3)C3—C21.420 (2)
C10—C111.380 (2)C3—H3A0.9300
C10—H10A0.9300C2—H2A0.9300
C4—C31.325 (2)C8—H8A0.9600
C4—C51.488 (2)C8—H8B0.9600
C13—C121.375 (2)C8—H8C0.9600
C13—N31.459 (2)
C4—O—C1105.97 (13)C4—C5—H5A110.0
C7—N1—N2108.34 (13)C6—C5—H5A110.0
C9—N2—N1118.80 (12)C13—C12—C11117.03 (16)
C9—N2—C5125.31 (13)C13—C12—H12A121.5
N1—N2—C5111.64 (12)C11—C12—H12A121.5
N2—C9—C14120.55 (14)C7—C6—C5103.00 (13)
N2—C9—C10120.96 (14)C7—C6—H6A111.2
C14—C9—C10118.47 (14)C5—C6—H6A111.2
C13—C14—C9118.59 (15)C7—C6—H6B111.2
C13—C14—H14A120.7C5—C6—H6B111.2
C9—C14—H14A120.7H6A—C6—H6B109.1
N1—C7—C8121.87 (16)C2—C1—O110.60 (15)
N1—C7—C6113.46 (15)C2—C1—H1B124.7
C8—C7—C6124.64 (16)O—C1—H1B124.7
C11—C10—C9120.67 (16)C12—C11—C10121.50 (17)
C11—C10—H10A119.7C12—C11—H11A119.3
C9—C10—H10A119.7C10—C11—H11A119.3
C3—C4—O109.50 (15)C4—C3—C2107.27 (16)
C3—C4—C5134.10 (17)C4—C3—H3A126.4
O—C4—C5116.37 (14)C2—C3—H3A126.4
C12—C13—C14123.72 (16)C1—C2—C3106.65 (16)
C12—C13—N3119.04 (15)C1—C2—H2A126.7
C14—C13—N3117.24 (15)C3—C2—H2A126.7
O2—N3—O1122.13 (17)C7—C8—H8A109.5
O2—N3—C13118.76 (15)C7—C8—H8B109.5
O1—N3—C13119.11 (17)H8A—C8—H8B109.5
N2—C5—C4112.93 (12)C7—C8—H8C109.5
N2—C5—C6100.18 (13)H8A—C8—H8C109.5
C4—C5—C6113.50 (14)H8B—C8—H8C109.5
N2—C5—H5A110.0
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C12—H12A···O1i0.932.513.311 (2)144
Symmetry codes: (i) −x+2, −y+1, −z+1.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
C12—H12A···O1i0.932.513.311 (2)144
Symmetry codes: (i) −x+2, −y+1, −z+1.
Acknowledgements top

The authors would like to express their deep appreciation to the Start-up Fund for PhDs of the Natural Scientific Research of Zhengzhou University of Light Industry (No.2005001) and the Fund for Natural Scientific Research of Zhengzhou University of Light Industry, China (000455).

references
References top

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